Quantum Monte Carlo Study of Symmetry Breaking in a Double-Well Chain

  • J. E. Gubernatis
  • D. K. Campbell
  • Xidi Wang

Abstract

We report the results of a quantum Monte Carlo simulation of a double-well chain. This chain is a system of particles that move on a lattice of symmetric, double-well potentials which are coupled harmonically to one another. The physical properties of this system are invariant, like those of the the Ising model, under the symmetry operations of the Z 2 group. In this case, changing the sign of the displacement variables leaves the energy unchanged and leads to a doubly-degenerate ground-state. Classically, this symmetry is always broken, and the particles all sit in the left- or the right-hand side of their wells. Quantum mechanically, however, we find that below a critical value of the double-well coupling constant the symmetry is restored by quantum fluctuations.

Keywords

Alamos National Laboratory Quantum Fluctuation Monte Carlo Step Metropolis Algorithm Quantum Monte Carlo Simulation 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

Preview

Unable to display preview. Download preview PDF.

Unable to display preview. Download preview PDF.

References

  1. 1.
    E. Fradkin and J. E. Hirsch, Phys. Rev B27: 1680 (1982); J. E. Hirsch and E. Fradkin, Phys. Rev. B27: 4032 (1983).ADSGoogle Scholar
  2. 2.
    R. Dashen, B. Hasslacher, and A. Neveu, Phy. Rev. D10: 4114, 4139 (1974).ADSGoogle Scholar
  3. 3.
    For example, R. W. Jansen, R. Bcrtoncini, D. A. Pinnick, A. I. Katz, R. C. Hanson, O. F. Sankey and M. O’Keeffe, Phys. Rev. B35: 9830 (1987).ADSGoogle Scholar
  4. 4.
    R. P. Feynman and A. R. Hibbs, Quantum Mechanics and Path Integrals, McGraw-Hill, New York (1965).MATHGoogle Scholar
  5. 5.
    M. Creutz and B. Freedman, Ann. Phys. 132: 427 (1981).MathSciNetADSCrossRefGoogle Scholar
  6. 6.
    A. Milchev, D. W. Heermann and K. Binder, J. Stat.Phys. 44: 749 (1986).ADSCrossRefGoogle Scholar
  7. 7.
    R. Toral and A. Chakrabari, Phys. Rev. B42: 2445 (1990).ADSGoogle Scholar
  8. 8.
    S. Duane, Nucl. Phys. B257: 652 (1985); S. Duane and J. B. Kogut, Nucl. Phys. B275: 398 (1986).ADSCrossRefGoogle Scholar
  9. 9.
    W. H. Press, B. R. Flannery, S. A. Teukolsky, and W. T. Vetterling, Numerical Recipes, Cambridge Press, Cambridge (1986), p. 631.Google Scholar
  10. 10.
    K. Binder, in Applications of the Monte Carlo Method in Statistical Physics, Springer-Verlag, Berlin (1984), Chap. 1.MATHCrossRefGoogle Scholar
  11. 11.
    K. Binder, Z. Phys. B 43: 119 (1981); Phys. Rev. Lett. 47: 693 (1981).ADSCrossRefGoogle Scholar
  12. 12.
    A. M. Ferrenberg and R. Swendsen, Phys. Rev. Lett. 61: 2635 (1988); Phys. Rev. Lett. 63: 1195 (1989).ADSCrossRefGoogle Scholar
  13. 13.
    Xidi Wang, D. K. Campbell, J. E. Gubernatis, “Symmmetry breaking in a quantum double-well chain,” unpublished.Google Scholar
  14. 14.
    Rajiv R. P. Singh and G. A. Baker, Jr., Phys. Rev. Lett. 61: 1 (1991).MathSciNetADSCrossRefGoogle Scholar
  15. 15.
    Xidi Wang, D. K. Campbell, J. E. Gubernatis. G. A. Baker, Jr., “Conformai charge of the two-dimensional ϕ4 field theory,” unpublished.Google Scholar
  16. 16.
    G. A. Baker, Jr., and J. D. Johnson, J. Phys. A17: L275 (1984).MathSciNetADSGoogle Scholar
  17. 17.
    A. D. Bruce, J. Phys. A18: L873 (1985).ADSGoogle Scholar

Copyright information

© Springer Science+Business Media New York 1992

Authors and Affiliations

  • J. E. Gubernatis
    • 1
  • D. K. Campbell
    • 2
  • Xidi Wang
    • 2
  1. 1.Theoretical DivisionLos Alamos National LaboratoryLos AlamosUSA
  2. 2.Center for Nonlinear StudiesLos Alamos National LaboratoryLos AlamosUSA

Personalised recommendations